chapter 4 transient stability margin of scig in...
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CHAPTER 4
TRANSIENT STABILITY MARGIN OF SCIG IN WIND
FARM USING STATCOM
4.1 INTRODUCTION
Angular stability assessment of WEG is one of the main issues in
power system security and operation. Rotor speed stability refers to the ability
of an induction machine to remain connected to the electric power system and
running at a mechanical speed close to the speed corresponding to the actual
system frequency after being subjected to a disturbance (Kanabar 2008). In
practice, overspeed protection circuit disconnects the WEG from the grid
when its speed exceeds 1.2pu. From the power quality study undertaken in
one 110kV/11kV substation at Anthiyur windfarm it was observed that nearly
60% of power quality issues in windfarms are contributed by voltage
sags,29% by voltage swells,8% by transients and 3% by interruptions
(Thirumoorthy 2009). Normally, LVRT requirements are stringent in regions
with high penetration of wind power. In order to promote the integration of
wind farms into the electrical network, FACTS are widely used. STATCOM
is one of them (Hingorani 2000). STATCOM stimulates voltage stability by
reactive power regulation. STATCOM provides or absorbs reactive power to
or from the grid to compensate small voltage variations at PCC. Many studies
show that STATCOM helps the wind farm to stabilize voltage especially after
a voltage dip occurs. With regard to maintaining the short term voltage
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stability, all grid codes demand that the voltage in the transmission power grid
is re-established without subsequent disconnection of large wind farms.
In this chapter, the effect of STATCOM on the transient stability
margin of SCIG is studied under different penetration levels in the event of
unbalanced or balanced fault in the grid. The performance of WEG with
STATCOM is studied using MATLAB/Simulink taking into account the
nature of the load and the results are presented.
4.2 WIND FARM STABILITY AND REACTIVE POWER
COMPENSATION
A system experiences a state of voltage instability when there is a
progressive or uncontrollable drop in voltage magnitude after a disturbance,
increase in load demand or change in operating condition. The main factor,
which causes these unacceptable voltage profiles, is the inability of the
distribution system to meet the demand for reactive power (Alejandro Jurado
2009). The reactive power absorbed by the induction generator coupled to
wind turbine depends on the generator parameters and its operational points
(generated electric power, terminal voltage magnitude and slip). During the
fault, the generator speed is increased by the difference between
electromagnetic torque of SCIG and mechanical torque of WT. Once the fault
is cleared, the SCIG draws a large amount of reactive power from the grid
because of its high rotational speed. If the rotor accelerates faster than the
terminal voltage is restored, the reactive power consumption continues to
increase. This leads to a decrease in the terminal voltage and thus to a further
deterioration of the balance between mechanical and electrical power and to a
further acceleration of the rotor. Owing to this reactive power consumption, it
can happen that the terminal voltage recovers only relatively slowly after the
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fault is cleared. This decline in the electromagnetic torque causes a decrease
in the value of the CCT and hence the transient stability margin of SCIG.
4.3 EFFECT OF ADDITIONAL REACTIVE POWER SUPPORT
ON TRANSIENT STABILITY MARGIN OF SCIG
Figure 4.1 shows the torque-slip characteristics of a SCIG with two
different values of reactive power compensation (Kanabar 2008). For a given
set of machine parameters, the electromagnetic torque developed by the WEG
depends on the value of reactive power compensation .The additional value of
reactive power compensation will shift the torque-slip characteristic of SCIG
upwards. Consequently, the value of critical clearing slip will increase from
Scr1 to Scr2. which will enhance the rotor stability margin of SCIG. This, in
turn improves the CCT, which is in compliance with the LVRT requirements
in new grid code.
Figure 4.1 Torque-slip characteristic of SCIG with nominal and
additional reactive power
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4.4 ADVANTAGES OF STATCOM
Due to the low cost, shunt capacitors are the most commonly used
scheme to compensate reactive power in WEGs. Shunt capacitors are used in
banks and switched in and out of the circuit using contactors. Due to the surge
current taken by the capacitors while switching in, the lifetime of the
contactors is limited. The switching of capacitors excites transients and the
switching has to be done by keeping the transients minimum. Also the voltage
support provided will be discontinuous. STATCOM has better characteristics
than FC compensation and SVC. Reactive power output of STATCOM is
independent of the actual voltage at PCC. In contrast, the reactive output of
FC and SVC is proportional to the square of the voltage magnitude at PCC.
This makes the reactive power output from SVC to decrease rapidly when the
voltage at PCC decreases, thus reducing the system stability.
Nevertheless, FACTS systems provide faster and smoother
response to changes in wind farm voltage. On the other hand, shunt capacitors
give a poor response. Power quality issues in Anthiyur windfarm near
Udumalpet in Tamilnadu, show frequent failure of lightning arrestors and
studies show that switching out of capacitor may be one of the reasons which
would have caused the transients that leads to the failure of insulation.
4.5 STATCOM
4.5.1 Principle of Operation
During the last few decades, development of power electronics
technology has helped to propose and implement FACTS devices for
overcoming power quality problems in power system. A STATCOM is a
regulating device used on alternating current electricity transmission
networks. It can act as either as a source or sink of reactive power to an
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electricity network. When system voltage is low, the STATCOM generates
reactive power (STATCOM capacitive). When system voltage is high, it
absorbs reactive power (STATCOM inductive).The variation of reactive
power is performed by means of a VSC connected on the secondary side of
a coupling transformer. The VSC uses forced-commutated power electronic
devices GTOs, IGBTs or IGCTs which can be operated at high switching
frequency to synthesize a voltage from a DC voltage source. The
STATCOM can be operated in two different modes:
In voltage regulation mode (the voltage is regulated within
limits)
In VAR control mode (the STATCOM reactive power output is
kept constant)
When the STATCOM is operated in voltage regulation mode, it
implements the V-I characteristic shown in Figure 4.2.
Figure 4.2 STATCOM V-I characteristic
As long as the reactive current stays within the minimum and
minimum current values (-Imax, Imax) imposed by the converter rating, the
voltage is regulated at the reference voltage Vref. However, a voltage droop is
normally used (usually between 1% and 4% at maximum reactive power
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output), and the V-I characteristic has the slope indicated as shown in the
Figure 4.2.
4.5.2 Mathematical Model of STATCOM Control System
The STATCOM used is a standard 3-phase inverter with PWM
switching. The passive elements, namely, the series choke and the dc-bus
capacitor are designed to limit the ripple in the ac side current and dc bus
voltage of the STATCOM, respectively.
Figure 4.3 Schematic diagram of STATCOM connected to the grid
Figure 4.3 shows the schematic diagram of STATCOM connected
to grid. Assuming that the control of STATCOM is successful, the current
that will flow through R and L is equal to the reference current Ii .The voltage
that the inverter should generate is given below by applying Kirchhoff’s
voltage law. R is the equivalent loss resistance which includes winding
resistance, switch power loss etc. L is the filter inductance, Vg is the grid
voltage and Vi is the inverter output voltage before filtering (Arun
Karuppusamy 2007). Since the current references in the Synchronous
Reference Frame strategy are in the d-q plane, the equations are first written
in the R-Y-B plane and then they are transformed to the plane and
subsequently to the d-q plane. Applying KVL to the R-L circuit shown in
Figure 4.3, the Equations (4.1) to (4.3) are obtained:
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iaia ga ia
di (t)(t) (t) R.i (t) L.
dt(4.1)
ibib gb ib
di (t)(t) (t) R.i (t) L.
dt(4.2)
icic gc ic
di (t)(t) (t) R.i (t) L.
dt(4.3)
Converting the above equations to plane, Equation (4.4) to (4.5) are
obtained.
ii g i
di (t)(t) (t) R.i (t) L.
dt (4.4)
i
i g i
di (t)(t) (t) R.i (t) L.
dt(4.5)
In general, Equation (4.6) can be written for STATCOM.
ii g i
dIV V R.I L
dt(4.6)
As it is known that plane is related to d-q plane by the relation
given by Equation (4.7), Equation (4.8) is obtained.
( + j ) = (d cos - q sin ) + j ( d sin + q cos ) = (d + jq).e j
(4.7)
j
id iqj j j
id iq id iq gd gq
d i ji .ej .e R i ji .e L j .e
dt(4.8)
The above equation , when multiplied by e-j is transformed to d-q
plane. Since d-axis is aligned with grid voltage, Equation (4.9) to (4.10) are
obtained.
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idid id iq
diR.i L L.i | V |
dt(4.9)
iq
iq iq id
diR.i L L.i
dt (4.10)
From the above two Equations, the d axis and q axis currents Iid and
Iiq can be represented as shown in Figure 4.4.
Figure 4.4 Representation for d axis and q-axis currents of STATCOM
Where
id id iq' Li | V | (4.9)
iq iq id' Li (4.10)
Above mathematical equations can be represented as block diagram
shown in Figure 4.5, in which the d-axis and q-axis reference voltage vid and
viq of STATCOM are obtained. Reactive power control is achieved by control
of Iiq and active power control by control of Iid .
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Figure 4.5 Representation of d-axis and q-axis voltage at PCC
Similarly for DC bus voltage controller, Equation (4.11) can be
obtained.
Iid = C dVdc/dt + Vdc/R (4.11)
Figure 4.6 shows the representation for DC bus voltage controller
of STATCOM.
Figure 4.6 Representation of STATCOM DC bus voltage controller
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4.5.3 Design and Control of STATCOM
The design of a STATCOM has three broad sections (Arun
Karuppaswamy 2007):
1. Current reference generation (It involves computing the
reactive current absorbed by SCIG).
2. Design of the DC bus capacitor and inductor
3. Design of closed loop controller, that makes the STATCOM
current to follow the reference.
The first part of the design is to generate the current reference.
There are several methods to generate the current reference. The present study
is based on the application of co-ordinate transformations to separate the
active and reactive components of the current. The strategy used is the Vector
control method (Arun Karuppaswamy 2007). Once the current reference has
been generated, the next work is to find the values of DC capacitor and
inductor of STATCOM, according to the requirement of the reactive power
compensation.
The reactive current injected is controlled so as to obtain full rated
grid voltage before, during and after the fault. It is based on the measurement
of voltage at PCC. The voltage error signal is obtained by comparing the
actual and reference voltage, which is fed to a PI controller. There needs to be
another voltage controller to maintain a constant DC bus voltage. The
STATCOM current is continuously compared with reference current received
from two voltage controllers and error signal is fed into the Hysteresis
comparator.
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Hysteresis current control is a method of controlling a voltage
source inverter so that an output current is generated which follows a
reference current waveform. This method controls the switches in an inverter
asynchronously to ramp the current through an inductor up and down so that
it tracks a reference current signal. This scheme is employed for generation of
pulses to the STATCOM. This is a continuous current variable switching
current control scheme. The STATCOM current is continuously compared
with the reference current waveform and the error signal after amplification is
fed into the hysteresis comparator. The comparator changes state when the
error exceeds a preset value in positive and negative directions. The
comparator state switches is used to decide which of the switches should be
on and which of the switches should be off. When the STATCOM current
actually goes above the reference current by the comparator hysteresis band,
the comparator changes state. This state change is used to switch off the boost
switch and current ramps down. When the STATCOM current goes below the
reference current by comparator hysteresis band, it changes state again and
state change is used to turn the boost switch on. Thus the STATCOM current
is always maintained within half of the hysteresis band. A hysteresis current
controller is implemented with a closed loop control system and is shown in
diagrammatic form in Figure 4.7(a) (David 2009). An error signal, e(t), is
used to control the switches in an inverter. This error is the difference
between the desired current, iref(t), and the current being injected by the
inverter, iactual(t). When the error reaches an upper limit, the IGBTs are
switched to force the current down. When the error reaches a lower limit the
current is forced to increase. The minimum and maximum values of the error
signal are emin and emax respectively. The range of the error signal, emax –
emin, directly controls the amount of ripple in the output current from the
inverter and this is called the Hysteresis Band. The hysteresis limits, emin and
emax, relate directly to an offset from the reference signal and are referred to
as the Lower Hysteresis Limit and the Upper Hysteresis Limit. The current is
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forced to stay within these limits even while the reference current is changing.
The ramping of the current between the two limits is illustrated in Fig 4.7(b).
Figure 4.7 Block diagram and operational waveform of Hysteresis
current controller
Figure 4.8 shows the total control block diagram of the vector
control scheme for STATCOM.
Figure 4.8 Block diagram of the Vector Control Scheme for STATCOM
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4.6 SIMULATION RESULTS
One of the methods to meet the LVRT requirements is by providing
additional reactive power support which can improve the terminal voltage
during a disturbance. For the purpose of analysis, the system shown in Figure
2.7 is considered with VAR compensation as STATCOM. The SCIG acts as a
load requiring variable reactive power. It was found that SCIG is drawing a
reactive power of nearly 900kVAR during severe three phase to ground fault
with no VAR compensation. The STATCOM’s power rating is to be decided
based on the reactive power requirement. It is discussed in section 4.3, that
additional reactive power improves the transient stability margin of SCIG. A
STATCOM of 1000kVAR is assumed to be installed at PCC as SCIG is
drawing approximately 900kVAR during severe three phase to ground fault
without any compensation. Simulation studies have been carried out assuming
that the system is operating at full load and 12m/s wind speed. Different types
of faults are simulated at PCC. Simulations are repeated for the system with
1000kVAR FC compensation.
Table 4.1 shows the maximum reactive power (Q) consumption of
WEG, maximum SCIG speed and settling time after the fault for different
fault conditions with FC compensation and STATCOM compensation. The
slip of SCIG after the fault clearance is larger than that prior to the fault. The
larger the slip, the larger will be the reactive power demand of SCIG. Results
show that most of the parameters are reduced when 1000 kVAR STATCOM
is used for compensation instead of 1000 kVAR FC, which means that
STATCOM is responding faster than FC.
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Table 4.1 Comparison of FC compensation with STATCOM
compensation for different fault conditions at the wind speed of
12m/ s
FC compensation STATCOM compensationNature of
fault and
fault
duration
Maximum
Q (kVAR)
Maximum
SCIG
speed
(rad/s)
Settling
time
after the
fault (s)
Maximum
Q(kVAR)
Maximum
SCIG
speed
(rad/s)
Settling
time
after the
fault (s)
Single line to
ground fault
(600ms)
500 168 1.5 400 167 1.25
Double line
to ground
fault(100ms)
1080 175 1.25 920 178 0.8
Three phase
to ground
fault(50ms)
925 186 1 620 179 0.9
For considering the effect of wind penetration level on transient
stability of SCIG, the two machine system shown in Figure 3.6 is taken for
study with VAR compensation as STATCOM. Assuming that the system
under consideration is operating at full load, the transient stability of SCIG
under different fault conditions of various fault durations with STATCOM
compensation is studied.
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4.6.1 250 kW SCIG Connected to 2000kVA Alternator (Medium
Penetration)-Case 1
4.6.1.1 Single line to ground fault
A single line to ground fault is simulated at the instant of 2 seconds
from the start at PCC. The fault is cleared after 100ms. The wind speed is
assumed to be 10m/s, which is the normal case prevailing in practice.
Simulation is repeated for different fault durations and corresponding values
of the performance indices are given in Table 4.2. It is observed that for
longer duration faults, dip in DC link capacitor voltage is more. STATCOM
DC link voltage Vdc is maintained at 600V before and after fault. Alternator
speed and Vpcc settle at 1 pu.
Figure 4.9 shows the plots of the parameters for a fault duration of
625ms. From Figure 4.9 , it is inferred that grid code is satisfied for single line
to ground fault as the system returns to stable condition without getting
tripped for 625ms fault duration.
Table 4.2 Range of transients in different parameters at SCIG terminals
for single line to ground fault at PCC(case 1)
Fault
Duration(ms) ( rad/sec) P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
100 157.5-160.5 120-200 79-109 265-1800 0.98-1 576-643
625 156.6-160.8 119-200 75-109 265-1800 0.98-1 570-643
80
Figure 4.9 System performance indices for single line to ground fault of
625ms duration at PCC for a wind speed of 10m/s at full
load of 0.9 power factor lagging (case 1)
81
4.6.1.2 Double line to Ground fault
A double line to ground fault is implemented at PCC. Table 4.3
shows the results for double line to ground fault of different durations. During
the fault, the alternator speed varies over 0.99 to 1.03pu. For 100ms fault
duration, Vpcc and Vdc settle at 0.985pu and 600V respectively. For 400ms
fault, Vpcc and Vdc settle at respective values of 0.945 pu and 580V .For
500ms fault duration, Vpcc and Vdc settle at 0.94 pu and 570V respectively.
Figure 4.10 shows the plots for 100ms fault duration.
Table 4.3 Range of transients in different parameters at SCIG terminals
for double line to ground fault at PCC for a wind speed of
10 m/s(case 1)
Fault
duration(ms) ( rad/sec) P (kW)
Q
(kVAR)Te (Nm)
Vpcc
(pu)Vdc (V)
100 151.4-171-27 to
+330
-360 to
+590
+4370 to
-7075
0.39
to1.08390-917
200 151.4-171-28 to
+250
-510 to
+605
+4370 to
-7075
0.38 to
1.045400-910
400 151.5-188.5-27.5 to
308
-700 to
+625
+4370 to
-7075
0.36
to0.96400-805
500 151.5-202-55 to
210
-640 to
+600
+4370 to
-70750.36- 0.93 300-845
When the fault duration is increased to 550ms, SCIG speed
increases indefinitely and the system becomes unstable. Vpcc dips to 0.355pu
during fault and settles at 0.917pu after the fault. Figure 4.11(i) shows the
plots of and Te for 550ms double line to ground fault at PCC for a wind
speed of 10m/s at full load. But when the load demand is reduced to half, the
system retains its stability by returning to original condition. Alternator speed
settles at 1.017 pu. Vpcc, SCIG speed and Te respectively settle at 0.92pu,
171rad/s and 975Nm.
82
Figure 4.10 System performance indices for double line to ground fault
of 100ms duration at PCC for a wind speed of 10m/s at full
load of 0.9 power factor lagging (case 1)
83
At half load, even though the operating speed of SCIG is high, the
transient stability margin of SCIG is better than that with full load. This is
because of the fast response of STATCOM. Table 4.4 shows the parameter’s
variations for half load .Figure 4.11(ii) shows the plots of and Te
corresponding to this condition.
Figure 4.11(i) and Te for double line to ground fault of 550ms duration
at PCC for a wind speed of 10m/s at full load of 0.9 power
factor lagging (case 1)
Table 4.4 Range of transients in different parameters at SCIG terminals
for 550 ms double line to ground fault at PCC for a wind speed
of 10 m/s at half load of 0.9 power factor lagging (case 1)
Fault duration
(ms) (rad/s) P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
550159.6-
182
-25 to
+260
-550 to
+620
+5455 to -
87000.39-1 400-965
84
Figure 4.11(ii) and Te for double line to ground fault of 550ms duration
at PCC for a wind speed of 10m/s at half load of 0.9 power
factor lagging (case 1)
Figure 4.11(iii) and Te or double line to ground fault of 550ms duration
at PCC for a wind speed of 8m/s at full load of 0.9 power
factor lagging (case 1)
When the wind speed is reduced to 8m/s from 10m/s for 550ms
fault at full load, the system regains to original condition and the system
becomes stable. Table 4.5 shows the variations for 8m/s during fault
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condition. Figure 4.11(iii) shows the plots of and Te. Vdc, P,Q and Te
come to original values after the fault clearance.
Table 4.5 Range of transients in different parameters at SCIG terminals
for 550ms double line to ground fault at PCC for a wind speed
of 8 m/s at full load of 0.9 power factor lagging (case 1)
Fault duration
(ms) (rad/s) P(kW) Q(kVAR) Te(Nm) Vpcc(V) Vdc(V)
550145.8-
167.8
+145 to -
132
-450 to
+600
- 8050 to
+5370
0.39 to
1.065415-950
When the fault duration is increased to 625ms at half load of 0.9
power factor lagging, the system still returns to stable condition after the
clearance of the fault. SCIG speed, P, Vdc and Te respectively settle at
171rad/s,160kW,600V and 950Nm.Alternator speed settles at 1.01pu in 8s.
Vpcc settles at 0.905pu.Table 4.6 shows the transients during fault. Figure
4.12 shows the plots of and Te for this condition.
Figure 4.12 and Te for double line to ground fault of 625ms duration
at PCC for a wind speed of 10m/s at half load of 0.9 power
factor lagging (case 1)
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Table 4.6 Range of transients in different parameters at SCIG terminals
for 625ms double line to ground fault at PCC for a wind speed
of 10 m/s at half load of 0.9 power factor lagging (case 1)
Fault duration
(ms) (rad/s) P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
625165.8-
187
-25 to
270
-550 to
+620
3120 to -
53800.39-0.995 385-885
4.6.1.3 Three phase to Ground fault
A three phase to ground fault at the generator terminals is
considered for the study. Table 4.7 shows the different parameter variations
and system becomes stable after the clearance of the fault. Alternator speed
varies over 0.96 to 1.055pu during fault. For 50ms, 100ms, 200ms and 250ms
fault durations, Vpcc settle at 1pu, 0.955 pu, 0.94 pu and 0.92 pu
respectively. Figure 4.13 shows the plots for 100ms fault.
Table 4.7 Range of transients in different parameters at SCIG terminals
for three phase to ground fault at PCC for a wind speed of 10
m/s at full load of 0.9 power factor lagging (case 1)
Fault duration
(ms) (rad/s) P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
50143.5-
179
-255 to
+410
-370 to
+200
+2700 to -
80000-1.075 350-835
100143.5-
180
-110 to
+355
-440 to
+200
+2700 to -
80250-1.075 288-868
200143.5-
203
-88 to
+253
-575 to
+200
+2700 to -
80300-0.985
240-
1310
250143.5-
211.5
-72 to
+222
-620 to
+200
+2700 to -
81000-0.865
200-
1545
87
Figure 4.13 System performance indices for three phase to ground fault
of 100ms duration at PCC for a wind speed of 10m/s at full
load of 0.9 power factor lagging (case 1)
88
When the fault duration is increased to 280ms duration, the system
becomes unstable for RL load of 0.9 power factor lagging. Figure 4.14(i)
shows the plots of Te and SCIG speed for this condition. If unity power factor
load is used for the same type and duration of fault and 10m/s wind speed, the
system retains its original condition and thereby stability is attained. Table 4.8
shows the variations for this condition. Figure 4.14(ii) shows the plots of Te
and SCIG speed.
Figure 4.14(i) and Te for three phase to ground fault of 280ms
duration at PCC for a wind speed of 10m/s at full load of
0.9 power factor lagging (case 1)
Table 4.8 Range of transients in different parameters at SCIG
terminals for three phase to ground fault at PCC for a wind
speed of 10 m/s at full load unity power factor (case 1)
Fault
duration
(ms)(rad/s)
P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
280215-
139
-79 to
+225
-640 to
+220
+2790 to -
85200-1.06
220-
1555
When the fault duration is increased to 300ms, the system becomes
unstable. For same type of fault and duration, when the wind speed is reduced
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from 10m/s to 8m/s, the system remains stable. Table 4.9 shows the variations
during fault. After fault, Vpcc and SCIG speed settle at 0.92pu and 157rad/s
respectively.
Figure 4.14(ii) and Te for three phase to ground fault of 280ms
duration at PCC for a wind speed of 10m/s at full load of
unity power factor (case 1)
Table 4.9 Range of transients in different parameters at SCIG
terminals for three phase to ground fault at PCC for a wind
speed of 8 m/s at full load of 0.9 power factor lagging(case 1)
Fault
duration
(ms)(rad/s)
P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
300139-
175.5
-92 to
+230
-600 to
+200
+2600 to
-81800-1.025 240-860
4.6.2 250 kW SCIG Connected to 910kVA Alternator (High
Penetration)-Case 2
The penetration level of WEG is increased to 27% by connecting
the 250 kW SCIG to 910kVA alternator. Assuming that the load demand is
high, the simulation is carried out for different fault conditions.
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4.6.2.1 Single line to ground fault
A single line to ground fault is simulated at PCC.
Figure 4.15 System performance indices for single line to ground fault of
100ms duration at PCC for a wind speed of 10m/s at full
load of 0.9 power factor lagging(case 2)
91
Table 4.10 shows the variations for different fault durations.
Figure 4.15 shows the plots for 100ms fault. When compared to medium
penetration level, the range of transients is increasing for same type and
duration of fault. Vpcc settles at 1pu, 0.98pu and 0.975pu for fault durations
of 100ms, 400ms and 625ms respectively. Alternator speed settles at 1 pu for
all cases.
Table 4.10 Range of transients in different parameters at SCIG
terminals for single line to ground fault at PCC for a wind
speed of 10 m/s at full load of 0.9 power factor lagging (case 2)
Fault
duration
(ms)
(rad/s) P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
100 156.4-161.2 113-230 33-108 100-2100 0.955-1.035 524-671
400 155.8-161.2 113-230 45-109 100-2100 0.955-1.02 510-665
625 155-161 100-230 45-109 100-2100 0.955-1.01 525-665
4.6.2.2 Double line to ground fault
A double line to ground fault is implemented at PCC. Table 4.11
shows the parameter variations for double line to ground fault of different
durations. Figure 4.16 shows the plots for 100ms fault. Vpcc settle at 0.955pu,
0.95pu and 0.945pu respectively for 100ms, 200ms and 250ms faults. All
other parameters return to pre fault values.
Table 4.11 Range of transients in different parameters at SCIG
terminals for double line to ground fault at PCC for a wind
speed of 10 m/s at full load of 0.9 power factor lagging (case 2)
Fault
duration
(ms)(rad/s)
P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
100147-175.5
-58 to305
-300 to+525
+4750 to -8300
0.375-1.07 285-1080
200147-193.5
-30 to255
-440 to+525
+4750 to -8330
0.33-1.03 310-893
250 147-201-30 to220
-450 to+520
+4750 to -8330
0.32-0.99 250-820
92
Figure 4.16 System performance indices for double line to ground fault
of 100ms duration at PCC for a wind speed of 10m/s at full
load of 0.9 power factor lagging (case 2)
93
When the fault duration is increased to 300ms, the SCIG speed
increases indefinitely and becomes unstable. Figure 4.17(i) shows the plots of
Te and SCIG speed.. But, for the same fault duration, when the wind speed is
reduced to 8m/s from 10m/s, the system becomes stable. Table 4.12 shows the
results and Figure 4.17(ii) shows the plots of Te and SCIG speed. It shows
that lesser wind speed increases the transient stability margin of SCIG. Vpcc,
Vdc, SCIG speed and Te settle at 0.95pu, 600V, 157 rad/s and 450Nm
respectively.
Figure 4.17(i) and Te for double line to ground fault of 300ms duration
at PCC for a wind speed of 10m/s at full load of 0.9 power
factor lagging (case 2)
Table 4.12 Range of transients in different parameters at SCIG
terminals for double line to ground fault at PCC for a wind
speed of 8 m/s at full load of 0.9 power factor lagging (case 2)
Fault duration
(ms) (rad/s) P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
300148.5-
166.6
-85 to
+145
+560 to
-400
+3410 to
-5380
0.365-
1.075
370-
1115
94
Figure 4.17(ii) and Te for double line to ground fault of 300ms duration
at PCC for a wind speed of 8m/s at full load of 0.9 power
factor lagging(case 2)
4.6.2.3 Three phase to ground fault
A three phase fault is simulated at PCC. Variations in different
parameters during fault condition are given in the Table 4.13. Alternator
speed varies over 0.96 to 1.06pu for all faults. For 50ms, 100ms and 150ms,
Vpcc settle at 0.93pu, 0.915pu and 0.88pu respectively. Figure 4.18 shows the
plots for 50ms fault.
Table 4.13 Range of transients in different parameters at SCIG
terminals for three phase to ground fault at PCC for a wind
speed of 10 m/s at full load of 0.9 power factor lagging (case 2)
Fault
duration
(ms)
(rad/s) P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
50 145.5-178-165 to
+340
-295 to
+165
+2400 to
-72700-1.038 255-980
100 145.5-182-45 to
250
-360 to
+165
+2400 to
-72700-1.025 180-1050
150 145.5-193-35 to
240
-420 to
+165
+2400 to
-72700-0.93 60-1350
95
Figure 4.18 System performance indices for three phase to ground fault
of 50ms duration at PCC for a wind speed of 10m/s at full
load of 0.9 power factor lagging (case 2)
96
Figure 4.19(i) and Te for three phase to ground fault of 200ms
duration at PCC for a wind speed of 10m/s at full load of
0.9 power factor lagging (case 2)
When the fault duration is increased to 200ms, the system becomes
unstable at full load. Figure 4.19(i) shows the plots of Te and SCIG speed.
But at half load, for same fault, the system regains to original condition. It
shows that STATCOM is fast in producing counter balancing electromagnetic
torque of SCIG. Vpcc, SCIG speed, P,Q, Vdc and Te respectively settle at
0.92pu,173 rad/s, 160kW, 85kVAR, 560V and 950Nm. Table 4.14 shows the
results. Alternator speed settles at 1.01 pu in 9s. Figure 4.19(ii) show the plots
of Te and SCIG speed.
97
Figure 4.19(ii) and Te for three phase to ground fault of 200ms
duration at PCC for a wind speed of 10m/s at half load of
0.9 power factor lagging (case 2)
Table 4.14 Range of transients in different parameters at SCIG
terminals for three phase to ground fault at PCC for a wind
speed of 10 m/s at half load of 0.9 power factor lagging (case 2)
Fault
duration
(ms)(rad/s)
P(kW) Q(kVAR) Te(Nm) Vpcc(pu) Vdc(V)
200159-
213
-45 to
230
-500 to
+200
2725 to -
72000-0.935 35-1545
4.7 SUMMARY
This chapter analyzed the impact of penetration level and load
demand on the transient stability margin of SCIG coupled with WT in the
event of any unbalanced or balanced fault in the grid. It is seen that the
reactive power consumption of SCIG during fault is reduced when 1000
kVAR STATCOM is used for compensation instead of 1000 kVAR FC. Table
4.15 and Table 4.16 give the summary of the transient stability margin(in ms)
98
of SCIG for a wind speed of 10m/s at different loading conditions for medium
and high penetration levels respectively.
Table 4.15 Transient stability margin(in ms) of SCIG for a wind
speed of 10m/s at different loading conditions for medium
penetration
Fraction of LoadType of fault
Full load Half load
Nature of load RL load R load RL load R load
Single line to ground fault 625 625 625 625
Double line to ground fault 500 540 625 625
Three phase to ground fault 270 320 320 360
Table 4.16 Transient stability margin(in ms) of SCIG for a wind speed
of 10m/s at different loading conditions for high penetration
Fraction of LoadType of fault
Full load Half load
Nature of load RL load R load RL load R load
Single line to ground fault 625 625 625 625
Double line to ground fault 250 300 370 400
Three phase to ground fault 170 230 220 270
From Table 4.15 and Table 4.16, it can be seen that at half load, the
transient stability margin of SCIG is better than that with full load even
though the operating speed of SCIG is high. This is because of the fast
response of STATCOM. For highly resistive load, the transient stability
margin is increasing, as the resistance component of load offers damping
effect to rotor acceleration.